JPS5943603A - Distributed constant type filter - Google Patents

Distributed constant type filter

Info

Publication number
JPS5943603A
JPS5943603A JP15443482A JP15443482A JPS5943603A JP S5943603 A JPS5943603 A JP S5943603A JP 15443482 A JP15443482 A JP 15443482A JP 15443482 A JP15443482 A JP 15443482A JP S5943603 A JPS5943603 A JP S5943603A
Authority
JP
Japan
Prior art keywords
coupling
resonator
hole
filter
type filter
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP15443482A
Other languages
Japanese (ja)
Inventor
Toshio Nishikawa
敏夫 西川
Sadahiro Tamura
禎啓 田村
Hiroshi Tamura
博 田村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP15443482A priority Critical patent/JPS5943603A/en
Priority to US06/431,184 priority patent/US4464640A/en
Priority to GB08228112A priority patent/GB2109641B/en
Priority to DE19823236664 priority patent/DE3236664A1/en
Publication of JPS5943603A publication Critical patent/JPS5943603A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/205Comb or interdigital filters; Cascaded coaxial cavities
    • H01P1/2056Comb filters or interdigital filters with metallised resonator holes in a dielectric block

Abstract

PURPOSE:To make effective dielectric constant of dielectrics of each resonator to coincide with each other, by changing a position of a hole for adjusting degree of coupling in a distributed constant type filter. CONSTITUTION:In giving a deviation to a conventional coupling adjusting hole 54 toward the resonator 51 and a conventional coupling adjusting hole 55 toward the resonator 53, the conventional effective dielectric constants epsiloneff1 and epsiloneff2 are changed respetively to epsiloneff1' and epsiloneff2' (epsiloneff1>epsiloneff1', epsiloneff2<epsiloneff2') and a position obtaining epsiloneff1'=epsiloneff2' exists. The coupling adjusting holes provided at this position are 54', 55'. The effective dielectric constants of the dielectrics of resonators 51-53 are made to coincide by changing the position of the coupling adjusting holes in this way.

Description

【発明の詳細な説明】 この兄明は三段以上の分布定故形フィルタに関する。[Detailed description of the invention] This brother's work concerns a distribution-determined filter with three or more stages.

従来、収1 [] (] kAHZ城のフィルタとし”
Cば、LO」(撤回il!8を用いたものや空洞共振器
を1目(八たものかあつ/?lが、構造的に不安定ある
I^は複雑であったり、時性的に満足できな(へ、調整
に手間がかかる、コストが引下げられな(八、などの問
題点があった。
Conventionally, the filter used was 1 [] (] kAHZ Castle.”
C, LO' (withdrawal!8 or cavity resonator), but structurally unstable I^ is complex or temporally unstable. There were problems such as being unsatisfactory (heh), it took a lot of effort to make adjustments, and the cost could not be reduced (hah).

このため、第1図に示すように、%J% ′B3.体ブ
ロノブロック11の貫通孔12,13を設け、これら貫
通孔12.1ろの内面に導電膜14.15を設けるとと
もに」二記g重体ブロック11の四Ill面に嗜、市H
r)<、¥16を設け、上記貫通孔12.13の内面に
1没けたz、l]1.重膜14 + 15と、誘准体ブ
ロック11に設けた導電膜16と、その間に介在する誘
電体ブロック11とで、内、外導体間に固体iり′重体
が存在する同軸共1辰器を一対構成し、これら同軸共i
表器の間の誘電体ノ″ロック11 t’+ls分に結合
度調整孔17を設け、さら舒 に、図示しな髪へタフJ路と上記の共振ユニット、j−
を入力結合用コンデンサ18および出力結合用コンデン
サ19で夫々静心結合させるようにした、第2図に不ず
ような等価回路を有する分布定数形フィルタがある。
Therefore, as shown in FIG. 1, %J%'B3. The through holes 12 and 13 of the heavy body block 11 are provided, and a conductive film 14.15 is provided on the inner surface of these through holes 12.1.
r)<, ¥16 is provided, and z, l sunk into the inner surface of the through hole 12.13]1. The heavy films 14 + 15, the conductive film 16 provided on the dielectric block 11, and the dielectric block 11 interposed between them form a coaxial coaxial device in which a solid layer exists between the inner and outer conductors. A pair of coaxial i
A coupling degree adjustment hole 17 is provided in the dielectric lock 11 t'+ls between the front plates, and on the other hand, a tough J path and the above-mentioned resonance unit, j-
There is a distributed constant type filter having an equivalent circuit as shown in FIG. 2, in which the input coupling capacitor 18 and the output coupling capacitor 19 are statically coupled.

上記・′f)2図にお1/−I′C1216」二人力端
子、22は出力端子、26は入力結合静電容tit、、
24tよ出力結合靜市容計、25 、26 u E、’
4−波長共撮回jllδを堝中定収回路としC示したも
のである。従つ゛C1第1図の分布ノシ数形フィルター
1、’/’波長共振回路どうしは誘導結合され、外部N
路と1/4波長共振回路とが静電容叶結合されたフィル
タである。
・'f) 2 in figure 1/-I'C1216'' two-power terminal, 22 is the output terminal, 26 is the input coupling capacitance tit,
24t, output coupling, 25, 26 u E,'
The 4-wavelength co-imaging circuit jllδ is shown in C as a constant collection circuit in Sakanaka. Therefore, in the distributed number filter 1 in Figure 1, the '/' wavelength resonant circuits are inductively coupled to each other, and the external N
This is a filter in which a path and a 1/4 wavelength resonant circuit are capacitively coupled.

このような二段の分布定数形フィルタが存在する以上、
当然これを発展させ′C三段以上の分布定、7り形フィ
ルタを構成することが考えられる。
Since such a two-stage distributed constant filter exists,
Naturally, it is conceivable that this can be developed to construct a distribution-limiting, heptagonal filter with three or more stages.

第6図1は三段の場合の一例を示す。図にお1へて、5
1は一段目の同軸共振器間52は二段目の同IQb共振
器、53は三段目の同Φ111共振器である。54は一
段目と二段目間に位fjIt、する結合度調整孔、55
は二段目と三段目間に位置する結合度調整孔である。こ
のよう庁構造だと、二段目の同軸共振器52の両側には
結合度調整孔5.4.55があるが、一段目および三段
Y」の同軸共振器51.53では、片側にのみ結合度調
整孔54ある1凸ば55があるだ(・1である。このア
ンバランスな状態から、二段目の1′C・J軸共据器5
2の誘・−1i体の実効誘電率εeff2バlu l」
や三役1゛1の同軸共振器51.53の実効誘電率εQ
 rf Hより小;11−1値になつ′〔シ捷う。した
がつ゛〔その1までは二段目の共振器52の共振周波数
が高くなってしまlq、フィルタ背伸を得るトでの障害
となる。そのzt策とし〔二段目の共鴎’Any 5 
’:’の共振周波数を、一段目や三段目の共IlI←:
=51、S3のそれと等しくするべく、二段1」のJ(
ミ1辰P:、 s 2の誘電体部分だけ、材料を変え゛
C実効1.5多電・ドを高くしたり、第4図のように長
くすることが考えられるが実用的ではなIQo それゆえにこの発明の]」的は、各共振器の誘電体の実
効誘電率を一致させることである。
FIG. 61 shows an example of a three-stage case. Go to figure 1, 5
1 is the coaxial resonator of the first stage, 52 is the same IQb resonator of the second stage, and 53 is the same Φ111 resonator of the third stage. 54 is a coupling adjustment hole between the first stage and the second stage, 55
is a coupling degree adjustment hole located between the second and third stages. With such a structure, the coupling adjustment holes 5, 4, and 55 are provided on both sides of the second-stage coaxial resonator 52, but in the coaxial resonators 51, 53 of the first and third stages, there are holes on one side. There is only a coupling adjustment hole 54 and a convex protrusion 55 (1).From this unbalanced state, the second stage 1'
Effective dielectric constant εeff2balu l of di-1i body of 2
and the effective permittivity εQ of the triplex 1゛1 coaxial resonator 51.53
rf Less than H; becomes a value of 11-1. However, up to Part 1, the resonant frequency of the second stage resonator 52 becomes high lq, which becomes an obstacle to obtaining filter stretch. As for that zt strategy [Second stage co-gull'Any 5
Set the resonance frequency of ':' to the first and third stages' IlI←:
= 51, to make it equal to that of S3, J(
It is conceivable to change the material of only the dielectric part of 1.P:, s2 to increase the effective 1.5 current or to make it longer as shown in Figure 4, but this is not practical. Therefore, the object of this invention is to match the effective permittivity of the dielectric material of each resonator.

この発明の要旨は、誘電体ブロックに三つ以−4−の筒
状の孔を間隔をお1^゛C形成し、この孔の内周面に内
導体を形成するとともに、誘1E体7゛ロックの上記孔
を囲む西側面に外導体を形成し、内導体間に結合度調整
孔を設けることにより複数の同軸共振器間が誘導結合さ
れCなる分布定数形フィルタにお(^C1結合度調整孔
の位置を変えることにより、各共振器の誘電体の実効誘
電4kを一致させることである。
The gist of this invention is to form three or more cylindrical holes at intervals of 1^'C in a dielectric block, form an inner conductor on the inner peripheral surface of the holes, and form a dielectric body 7. By forming an outer conductor on the west side surrounding the above-mentioned hole of the lock and providing a coupling adjustment hole between the inner conductors, multiple coaxial resonators are inductively coupled to form a distributed constant filter (C1 coupling). The purpose is to match the effective dielectricity 4k of the dielectric of each resonator by changing the position of the degree adjustment hole.

以下にこの発明の一実施例を図ゝ而を参照しながら説明
する。なお前回と同一部分に1同−計号を付すことにす
る。
An embodiment of the present invention will be described below with reference to the drawings. Note that the same parts as last time will be marked with 1-double symbols.

従来の結合度)l・」整孔54を共限器51寄り虻、”
! fc、従来の結合度調整孔55を共1辰器53寄り
に、それぞれ偏位させC1^くと、従来の実効誘電率=
aff、 カεoff、’(CI3ff、〉εe:、’
f、’) ニ、従来ノ実効誘電率εeff2がεeごf
4’(=Gff2り+−’Qrf2 ’) Kなりεe
ff、’−ε5ff2’となる位置がある。この位1べ
に設けた結合度調整孔を54’ 、 55’  とする
Conventional degree of coupling) l・"The hole adjustment 54 is close to the common limiter 51,"
! If fc and the conventional coupling degree adjusting hole 55 are shifted closer to the 1st axis unit 53 and C1^, the conventional effective dielectric constant =
aff, kaεoff,'(CI3ff,〉εe:,'
f,') D. The conventional effective permittivity εeff2 is εegof
4'(=Gff2+-'Qrf2') K becomes εe
There is a position where ff, '-ε5ff2'. The degree of coupling adjustment holes provided at this point are designated as 54' and 55'.

第6図は四段の、14合の例であり、三段の1局合と同
様で、従来の結合度調整孔65.67をスJtぞれ共揚
器61,64寄りに偏位させ’C1^くと、従来の実効
rJ rll率ε9ff、 カε−+ff+’(aef
f+>εeff、’)(,4従来(7”) 11効誘t
li率εaff、カεeff2’(ceff、!<。e
ff2’)ニiす、εeff、1’−=+:ef f2
’となるr立置4がある。
Fig. 6 shows an example of a four-stage, 14-coupling case, which is similar to a three-stage, one-coupling case, in which the conventional coupling degree adjustment holes 65 and 67 are shifted toward the mutual lifters 61 and 64, respectively. 'C1^, the conventional effective rJ rll rate ε9ff, Ka ε-+ff+'(aef
f+>εeff,')(,4 Conventional (7") 11 Effect induction t
li rate εaff, Ka εeff2'(ceff,!<.e
ff2') Nisu, εeff, 1'-=+:ef f2
' There is an r standing 4.

この位置に1、りけた結合度調整孔を65′、67′と
する。このように本発明は三段以上のフィルタに有効で
ある。
The coupling adjustment holes 1 and 65' and 67' are inserted at this position. As described above, the present invention is effective for filters having three or more stages.

なお、どの結合度調整孔の位置をかえるかは任意である
。                   4゜また、
この発明は、実施例で述べたコモラインタイプの分布定
数形フィルタのみならず、インタデジタルタイプの6+
15定数形フイルタにも適用できる。
Note that the position of which coupling degree adjustment hole is changed is arbitrary. 4゜Also,
This invention applies not only to the distributed constant type filter of the Comoline type described in the embodiment, but also to the 6+ type of interdigital type filter.
It can also be applied to a 15 constant type filter.

以上の実施例からもあきらかなように、この発明は、誘
電体ブロックに三つ以上の筒状の孔を間隔をお14−[
形成し、この孔の内周面に内導体を形成するとともに、
誘電体ブロックの上記孔を囲む西側面に外導体を形成j
〜、内導体間に結合度、蘭学孔を設けることにより複数
の同軸共振器間が誘導結合されてなる分布定数形フィル
タにお1w′(、結合度調整孔の立置を変えることによ
り、各共振器の誘′重体の実効誘電を率を一致させたか
ら、誘′11す体ブロックの形状を凹凸にしたり、一部
材料をかえたりすることなく、簡乍な対策で各共振器の
実効誘電率を一致させることができる。な粋、さらVこ
考え方を一歩進め、積極的に結合度調整孔の設iff位
14を変えることにより、各共振器の実効誘電率を互(
八に異なる任意の値だ定めることができる。
As is clear from the above embodiments, the present invention provides three or more cylindrical holes in a dielectric block at intervals of 14-[
and forming an inner conductor on the inner peripheral surface of this hole,
Form an outer conductor on the west side surrounding the above hole of the dielectric block.
~, 1w' (by changing the vertical position of the coupling degree adjustment hole, each Since the effective dielectric constants of the dielectric bodies of the resonators are matched, the effective dielectric constant of each resonator can be easily adjusted without making the shape of the dielectric block uneven or changing some of the materials. By taking this idea one step further and actively changing the setting point 14 of the coupling adjustment hole, the effective permittivity of each resonator can be made to match.
Any value different from eight can be defined.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の分布定数形フィルタの縦断面図、’;:
’K 2図は・■1図の分イ[定数J1シフィルタの4
両回路図、第ろ図はフィルタユニットの平面図、第4図
ンよフィルタユニットの斜視図、第5図は本発明実施t
lJの平面ドj1第6図は(へ1一つの実施例の平面ト
l O 11ば11奔1′tt体ブロック、51〜53および6
1〜6A(□;、f:、匈市体共4練重体54955 
および65゛〜67’は活計1t’):、H14整孔で
ある。 (♀許出願人 株式会社  ←r t:+、+ 4v4住所第 5国 防 4 霞 括 タ 図 有)  乙  ロ −12
Figure 1 is a vertical cross-sectional view of a conventional distributed constant filter.
'K Figure 2 is -■ Figure 1's part I [4 of constant J1
In both circuit diagrams, Figure 4 is a plan view of the filter unit, Figure 4 is a perspective view of the filter unit, and Figure 5 is a diagram showing the implementation of the present invention.
Figure 6 shows the planar plane of lJ (to 1) of one embodiment.
1-6A (□;, f:, Xiongshi body 4 kneaded body 54955
and 65' to 67' are 1t' in total): H14 hole-forming. (♀ Applicant Co., Ltd. ← r t: +, + 4v4 Address No. 5 National Defense 4 Kasumikata Diagram) Otsu Ro-12

Claims (1)

【特許請求の範囲】[Claims] 誘、(を体ブロックに三つ5以上の筒状の孔を間隔を」
、−hで形成し、この孔の内周面に内導体を形成すると
ともに、誘rii体ブロックの一]二記孔を囲む四側さ
れCなる分布4辷故形フイルタにおい′C1結合度にj
、′3整孔の位置を変えることにより、各共振器の誘1
)1体の実効Jj ’ijj率を一致させることを特徴
とする分布4辷故形フイルタ。
(The body block has three or more cylindrical holes spaced apart from each other.)
, -h, and an inner conductor is formed on the inner circumferential surface of this hole, and a filter with a distribution of C on all four sides surrounding the dielectric block's two holes is formed with a degree of C1 coupling. j
, '3 By changing the position of the hole, the induction of each resonator is
) A distribution quadratic error shape filter characterized by matching the effective Jj 'ijj rates of one body.
JP15443482A 1981-10-02 1982-09-03 Distributed constant type filter Pending JPS5943603A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP15443482A JPS5943603A (en) 1982-09-03 1982-09-03 Distributed constant type filter
US06/431,184 US4464640A (en) 1981-10-02 1982-09-30 Distribution constant type filter
GB08228112A GB2109641B (en) 1981-10-02 1982-10-01 Distributed constant type filter
DE19823236664 DE3236664A1 (en) 1981-10-02 1982-10-04 DISTRIBUTION CONSTANT TYPE FILTER

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15443482A JPS5943603A (en) 1982-09-03 1982-09-03 Distributed constant type filter

Publications (1)

Publication Number Publication Date
JPS5943603A true JPS5943603A (en) 1984-03-10

Family

ID=15584100

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15443482A Pending JPS5943603A (en) 1981-10-02 1982-09-03 Distributed constant type filter

Country Status (1)

Country Link
JP (1) JPS5943603A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6354804A (en) * 1986-08-26 1988-03-09 Oki Electric Ind Co Ltd Dielectric filter
JPH07162205A (en) * 1993-10-08 1995-06-23 Electron & Telecommun Res Inst Dielectric filter

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5717201A (en) * 1980-07-07 1982-01-28 Fujitsu Ltd Dielectric substance filter

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5717201A (en) * 1980-07-07 1982-01-28 Fujitsu Ltd Dielectric substance filter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6354804A (en) * 1986-08-26 1988-03-09 Oki Electric Ind Co Ltd Dielectric filter
JPH07162205A (en) * 1993-10-08 1995-06-23 Electron & Telecommun Res Inst Dielectric filter

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